Gas: Definition, Law, Formula, Equation, Examples, Questions

Gas: Definition, Law, Formula, Equation, Examples, Questions

Shivani PooniaUpdated on 02 Jul 2025, 07:59 PM IST

Matter has no fixed shape or volume. Like fluids but unlike solids, gases have no fixed shape and take the volume of the container. This expansion takes place because gas molecules are far apart and moving in a random manner. This behavior is described by the kinetic theory of gases, which says that the gas molecules are constantly moving, with continuous collisions between themselves and with the walls of the container.

This Story also Contains

  1. The Gaseous State
  2. Characteristics of Gas
  3. Some Solved Examples
  4. Summary
Gas: Definition, Law, Formula, Equation, Examples, Questions
Gas

The Gaseous State

Gases and their properties play an important role in our daily lives. Our atmosphere consists Of a Mixture Of gases like dioxygen, dinitrogen, carbon dioxide, water vapors, etc. These gases shield us from harmful radiation. Life is supported by the dioxygen in the air that we breathe. Plants need carbon dioxide for photosynthesis.
There are in total eleven elements in the periodic table that exist as gases under normal conditions.

The composition of gases is always from non-metal eg. O2, N2, He2, Cl etc.

Following are the few physical properties of the gaseous state :

(i) The volume and shape of gases are not fixed. These assume the volume and shape of the container.

(ii) The thermal energy of gases >> molecular attraction.

(iii) Gases have infinite expansibility and high compressibility.

(iv) Gases exert pressure equally in all directions

(v) Gases have a much lower density than solids and liquids due to negligible intermolecular forces.

vi) Gas mix evenly with other gases or their mixtures are homogeneous in composition.

Characteristics of Gas

There are certain parameters or measurable properties which are used to describe the characteristics of gases

  • Volume (V): The volume of the container is the volume of the gas sample as gases occupy the entire space available to them.
    Pressure (P): Pressure Of the gas is the force exerted by the gas per unit area on the walls of the container in all directions.
    $\begin{aligned} & \text { S.I unit }=\text { pascal }(\mathrm{Pa}) \\ & 1 \mathrm{~Pa}=1 \mathrm{Nm}^{-2} \\ & 1 \mathrm{~atm}=1.013 \times 10^5 \mathrm{~Pa} \\ & \text { Conversions } \\ & 1 \mathrm{bar}=10^5 \mathrm{~Pa}=0.987 \mathrm{~atm} \\ & 1 \mathrm{~atm}=760 \mathrm{~mm} \mathrm{Hg} \\ & 1 \mathrm{~atm}=760 \text { torr } \\ & 1 \mathrm{~atm}=1.013 \times 10^5 \mathrm{~Pa}\end{aligned}$

    Temperature: It is the measure of hotness of the system and energy of the system.
  • $\begin{aligned} & \text { S.I unit }=\mathrm{m}^3 \\ & \text { C.G.S. unit }=\mathrm{cm}^3 \\ & \text { Commonly used unit }=\mathrm{L} \\ & 1 \mathrm{~L}=1000 \mathrm{~mL} \\ & 1 \mathrm{~mL}=10^{-3} \mathrm{~L} \\ & 1 \mathrm{~m}^3=10^3 \mathrm{dm}^3 \\ & 1 \mathrm{~m}^3=10^3 \mathrm{~L} \\ & 1 \mathrm{~m}^3=10^6 \mathrm{~cm}^3 \\ & 1 \mathrm{~m}^3=10^6 \mathrm{~mL}\end{aligned}$
  • $
    \begin{aligned}
    & \text { S.I unit }=\text { kelvin }(\mathrm{K}) \\
    & \mathrm{K}={ }^o \mathrm{C}+273
    \end{aligned}
    $
    ${ }^{\circ} \mathrm{C} \rightarrow$ centigrade degree or Celsius degree

Mass: The mass of a gas can be determined by weighing the container in which the gas is enclosed and again weighing the container after removing the gas. The mass of the gas is related to the number of moles of the gas i.e.Moles of gas $(\mathrm{n})=\frac{\text { Mass in grams }}{\text { Molar mass }}=\frac{\mathrm{m}}{\mathrm{M}}$

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Some Solved Examples

Example 1:
A gas occupies a volume of 500 mL at 27°C and 1 atm pressure. What will be its volume at 47°C and 1 atm pressure?

Solution:
Given:

- Initial volume (V1) = 500 mL
- Initial temperature (T1) = 27°C = 27 + 273 = 300 K
- Final temperature (T2) = 47°C = 47 + 273 = 320 K
- Pressure remains constant at 1 atm

Using the formula: V1/T1 = V2/T2
V2 = (V1 × T2) / T1
V2 = (500 mL × 320 K) / 300 K
V2 = 533.33 mL

Therefore, the volume of the gas at 47°C and 1 atm pressure is 533.33 mL.

Example 2:
A gas occupies a volume of 2 L at 27°C and 1 atm pressure. What will be its volume at 47°C and 0.5 atm pressure?

Solution:
Given:

- Initial volume (V1) = 2 L
- Initial temperature (T1) = 27°C = 27 + 273 = 300 K
- Final temperature (T2) = 47°C = 47 + 273 = 320 K
- Initial pressure (P1) = 1 atm
- Final pressure (P2) = 0.5 atm

Using the formula: (V1 × P1) / T1 = (V2 × P2) / T2
V2 = (V1 × P1 × T2) / (T1 × P2)
V2 = (2 L × 1 atm × 320 K) / (300 K × 0.5 atm)
V2 = 4.27 L

Therefore, the volume of the gas at 47°C and 0.5 atm pressure is 4.27 L.

Example 3:
A gas occupies a volume of 1 L at 27°C and 1 atm pressure. How many moles of the gas are present?

Solution:
Given:

- Volume (V) = 1 L = 1000 mL
- Temperature (T) = 27°C = 27 + 273 = 300 K
- Pressure (P) = 1 atm

Using the ideal gas equation: PV = nRT
Where:
- R = 0.082057 L⋅atm⋅mol−1⋅K−1

n = (P × V) / (R × T)
n = (1 atm × 1000 mL) / (0.082057 L⋅atm⋅mol−1⋅K−1 × 300 K)
n = 40.82 mol

Therefore, there are 40.82 moles of the gas present.

Example 4:
A gas occupies a volume of 2 L at 27°C and 1 atm pressure. How many molecules of the gas are present?

Solution:
Given:

- Volume (V) = 2 L = 2000 mL
- Temperature (T) = 27°C = 27 + 273 = 300 K
- Pressure (P) = 1 atm

Using the ideal gas equation: PV = nRT
Where:
- R = 0.082057 L⋅atm⋅mol−1⋅K−1

n = (P × V) / (R × T)
n = (1 atm × 2000 mL) / (0.082057 L⋅atm⋅mol−1⋅K−1 × 300 K)
n = 81.64 mol

1 mol = 6.022 × 1023 molecules (Avogadro's number)

Number of molecules = n × 6.022 × 1023
Number of molecules = 81.64 mol × 6.022 × 1023 molecules/mol
Number of molecules = 4.92 × 1025 molecules

Therefore, there are approximately 4.92 × 1025 molecules of the gas present.

Example 5:
A gas occupies a volume of 3 L at 27°C and 1 atm pressure. What will be its volume at 47°C and 2 atm pressure?

Solution:
Given:

- Initial volume (V1) = 3 L
- Initial temperature (T1) = 27°C = 27 + 273 = 300 K
- Final temperature (T2) = 47°C = 47 + 273 = 320 K
- Initial pressure (P1) = 1 atm
- Final pressure (P2) = 2 atm

Using the formula: (V1 × P1) / T1 = (V2 × P2) / T2
V2 = (V1 × P1 × T2) / (T1 × P2)
V2 = (3 L × 1 atm × 320 K) / (300 K × 2 atm)
V2 = 3.2 L

Therefore, the volume of the gas at 47°C and 2 atm pressure is 3.2 L.

Summary

Gas molecules travel very fast and far apart, which causes intermolecular forces to become negligible. These forces that keep them moving so fast, coupled with the spacing, give gases a very low density. Gases is that they are highly compressible. Whereas solids and liquids cannot so easily be compressed to exist in smaller volumes, this certainly is not the case for pressurized gases.

Frequently Asked Questions (FAQs)

Q: What is the significance of the Boltzmann distribution in gas behavior?
A:
The Boltzmann distribution describes the probability of finding particles
Q: How does the concept of mean free path change in a gas as pressure increases?
A:
As pressure increases in a gas, the mean free path decreases. This is because higher pressure means more gas particles in the same volume, leading to more frequent collisions between particles. The relationship is inverse: mean free path is inversely proportional to pressure. This concept is important in understanding gas transport properties like diffusion and thermal conductivity, especially in applications like vacuum technology and plasma physics.
Q: What is the significance of Avogadro's number in gas calculations?
A:
Avogadro's number (approximately 6.022 × 10²³) represents the number of particles (atoms, molecules, or formula units) in one mole of a substance. In gas calculations, it's crucial for converting between the number of particles and the number of moles. It also helps in understanding the concept of the molar volume of a gas, which is the volume occupied by one mole of an ideal gas at STP (approximately 22.4 L).
Q: How does the speed of sound in a gas relate to its temperature and molecular mass?
A:
The speed of sound in a gas is related to its temperature and molecular mass by the equation: v = √(γRT/M), where v is the speed of sound, γ is the ratio of specific heats (Cp/Cv), R is the gas constant, T is absolute temperature, and M is the molar mass of the gas. This relationship shows that sound travels faster in gases with higher temperatures or lower molecular masses, which is important in fields like acoustics and aerodynamics.
Q: What is the virial equation of state and how does it improve upon the ideal gas law?
A:
The virial equation of state is an improvement on the ideal gas law that accounts for non-ideal gas behavior. It's expressed as a power series in terms of 1/V or P: PV/nRT = 1 + B/V + C/V² + ..., where B, C, etc., are virial coefficients that depend on temperature and the specific gas. This equation provides a more accurate description of gas behavior over a wide range of conditions and can be truncated at different levels of accuracy as needed.
Q: How does the concept of reduced variables help in understanding gas behavior across different substances?
A:
Reduced variables are dimensionless quantities obtained by dividing actual variables (pressure, volume, temperature) by their critical values. For example, reduced temperature T(r) = T/T(c), where T(c) is the critical temperature. Using reduced variables allows for the comparison of gas behaviors across different substances. The principle of corresponding states suggests that all gases behave similarly when compared at the same reduced conditions, which is useful in predicting gas properties and behavior.
Q: What is the significance of the Linde technique in gas liquefaction?
A:
The Linde technique is a method used to liquefy gases based on the Joule-Thomson effect. It involves compressing a gas, cooling it, and then allowing it to expand rapidly, which causes further cooling. This process is repeated until the gas liquefies. The technique is significant because it allows for the liquefaction of gases with low critical temperatures, such as nitrogen and oxygen, which is crucial for industrial gas separation and storage.
Q: How does the concept of fugacity improve upon the ideal gas law for real gases?
A:
Fugacity is a measure of the tendency of a substance to escape from a phase. For an ideal gas, fugacity equals pressure, but for real gases, it differs. The concept of fugacity allows thermodynamic equations developed for ideal gases to be applied to real gases by replacing pressure with fugacity. It accounts for the non-ideal behavior of real gases, especially at high pressures, and is crucial in chemical engineering and thermodynamics calculations.
Q: What is Amagat's Law and how does it relate to gas mixtures?
A:
Amagat's Law states that the volume of a gas mixture is equal to the sum of the volumes that each gas would occupy if it were alone at the temperature and pressure of the mixture. Mathematically, V(total) = V₁ + V₂ + V₃ + ... This law complements Dalton's Law of Partial Pressures and is useful in calculating the properties of gas mixtures, especially when dealing with volumes rather than pressures.
Q: What is Brownian motion and how does it relate to gas particle behavior?
A:
Brownian motion is the random, erratic movement of particles suspended in a fluid (liquid or gas), caused by collisions with the fast-moving atoms or molecules in the fluid. In gases, this motion is a direct result of the constant, random movement of gas particles. Brownian motion provides evidence for the kinetic theory of gases and helps explain phenomena like diffusion and the equal distribution of gas particles throughout a container.